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84894388680
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-
-
84894388809
-
-
note
-
d × [-T/2, T/2] to vouchsafe the eigenfunction-eigenvalue properties that we shall assert. For finite area photodetectors and finite measurement intervals, however, the principal pathological cases that can occur in Eq. (25) arise from covariance functions that are delta correlated in space, time, or both. In Section 3 we shall see how such a case can be handled directly from Eq. (18), with a solution that can be understood from Eq. (25).
-
-
-
-
15
-
-
84894395924
-
-
note
-
Note that the cos(ωt) term in Eq. (47) can be phase shifted by an arbitrary amount without invalidating Eq. (48). Physically, this is because the spectrum analysis measurement is insensitive to radio-frequency (frequency ω) phase shifts.
-
-
-
-
16
-
-
0000022924
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Broad-band parametric deamplification of quantum noise in an optical fiber
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24244441257
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Yuen, H.P.1
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20
-
-
84894394136
-
-
note
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In anticipation of the photon-units formulation that we shall employ for the quantum theory to come, we are expressing the classical fields in these units too; see Ref. 4.
-
-
-
-
21
-
-
0001091458
-
Quantum propagation in a Kerr medium: Lossless, dispersionless fiber
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12 We shall eschew the inclusion of these temporal effects in our bulk Kerr medium example because our principal aim, in this section, is to develop quantum-mechanically consistent signal-field covariances with which to explore the issue of LO optimization. Our fiber FWM treatment, in Section 4, will specifically address the noninstantaneous Kerr nonlinearity.
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0003498504
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23
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0002716347
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Squeezing of pulses in a nonlinear interferometer
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84975636001
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Exact solution for quantum self-phase modulation
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25
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0011259171
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Quantum theory of nonlinear loop mirrors
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26
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0001091458
-
Quantum propagation in a Kerr medium: Lossless, dispersionless fiber
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L. G. Joneckis and J. H. Shapiro, "Quantum propagation in a Kerr medium: lossless, dispersionless fiber," J. Opt. Soc. Am. B 10, 1102-1120 (1993).
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27
-
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0004229088
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0009751525
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Boivin, L.1
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29
-
-
84894398326
-
-
note
-
R = 300 K than the 0.03 value of a typical fiber; cf. Ref. 12.
-
-
-
-
30
-
-
84894397454
-
-
note
-
H1(t)}.
-
-
-
-
32
-
-
84894388541
-
-
note
-
10
-
-
-
-
33
-
-
84894402051
-
-
note
-
min(0).
-
-
-
-
34
-
-
84975555074
-
Tunable optical frequency division using a phase-locked optical parametric oscillator
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0028382354
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Terahertz optical frequency comb generation and phase locking of an optical parametric oscillator at 665 GHz
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Brothers, L.R.1
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|